Stochastic models The former one is used to A random function Z Z

a summary of findings and suggestions for future enhancements in Section 4. 2. MODELS AND VARIOGRAMS 2.1 Random function and variogram From spatial statistics point of view, the spatial structure and variability revealed in SAR data can be modeled by a regionalized variable zx, which is simply considered as the realization of a random function Zx constructed at all points x of a given region D ⊂ R 2 , while Z={Zx : x ∈ D ⊂ R 2 } defines a random field on D. The SAR data have been translated into general datum for analyzing. A stationarity condition should be set up first. Let Zx be the second-order stationarity random function, then it is of the following properties, E Zx ⎡⎣ ⎤⎦= m Cov Z x,Zx + h ⎡⎣ ⎤⎦= Ch 1 where m is the expectation value of Zx and Ch is the covariance function for all pairs of pixels x and x+h. When h = 0, Cov Z x , Z x + h ⎡ ⎣ ⎤ ⎦ = Cov Z x , Z x ⎡ ⎣ ⎤ ⎦ = Var Z x ⎡ ⎣ ⎤ ⎦ = C 0 2 he covariance function divided by the variance is called the correlation function C C h h = ρ 3 Under second-order stationarity assumption, the second-order variogram γ 2 h of Zx, which describes the variability between the intensity values of two pixels separated with h, is γ 2 h = 1 2 Var Z x + h − Zx ⎡⎣ ⎤⎦ 4 From Eqs. 1 and 2 Schabenberger Gotway, 2005, 2 1 [ ] 2 1 [ ] 2 1 [ ] 2 [ , ] [ ] Var Z Z Var Z Var Z Cov Z Z Var Z C C C γ = + − = + + − + = − = − h x h x x h x x h x x h h 5 In isotropic stochastic processes, the covariance is a function of the Euclidian distance h=||h|| only, that is, Ch = Ch. σ 2 is the variance of Zx. As a result, Eq. 5 can be simplified as follows, 2 2 h C h − = σ γ 6 Fig.1 shows the relationship between Ch and γ 2 h. R is the largest distance between two relative positions; Sill is the limitation value of γ 2 h, its equal to C0. When h exceeds the range, Ch tends to zero and γ 2 h is stabilized. It means that data separated by a distance larger than the R are uncorrelated. The R is an important parameter related to the spatial scale of the data Feng, 2008. It can be used to reflect the floe size of sea ice, so how to estimate R from data images accurately is a significant part of this method. For a given random function Zx, under second-order stationarity assumption and in isotropic stochastic processes, its first-order variogram γ 1 h is defined as follow Chiles Delfiner, 1999 γ 1 h = 1 2 E Z x + h − Zx ⎡ ⎣ ⎤ ⎦ 7 where γ 1 h is seen as first-order moment. When h approaches its range R, the value of γ 1 h tends to be constant. The first- and second-order variograms will both be used to characterize the spatial structures and their validities and accuracies will be compared in the following sections.

2.2 Stochastic models

In order to characterize the sea ice spatial structures, SAR intensity images are considered as a combination of two stochastic second-order stationary models. According to the SAR data properties Keith et al. 2006 and the distribution properties of sea ice, we build multi-Gamma model Z g x and Poisson mosaic model Z m

x. The former one is used to

characterize continuous variations corresponding to the background of sea ice, the other is a tessellation model in which the image domain is randomly separated into non-overlapping cells to simulate the real sea ice areas. Chilès Delfiner, 1999. 2.2.1 Bivariate Gamma model Z g

x: A random function

Z g x is said to be a bivariate Gamma random function if the vector Z = Z g

x, Z

g x + h for x, x + h ∈ D is distributed according to a bivariate Gamma distribution. The bivariate Gamma distribution on R 2 has been defined in several forms. Most of them exploit various properties of the univariate Gamma distribution to construct bivariate families Kotz et al., 2000. In this paper, bivariate Gamma distribution of random vector Z = Z g

x, Z

g x + h in R 2 is defined by its moment generating function or Laplace transform, which is defined with an affine polynomial Bernardoff, 2006. We use an affine polynomial 2 1 2 2 1 1 θ ρθ β βθ βθ + + + = θ p 8 where the parameters satisfy the conditions: β 0 and 1 ρ

0. Then the moment of the generating function of Z can be defined as